Simulation of convectiveconductiveradiative heat transfer in a cooling basin - PowerPoint PPT Presentation

1 / 17
About This Presentation
Title:

Simulation of convectiveconductiveradiative heat transfer in a cooling basin

Description:

A Numerical simula-tion of three-dimensional hydrothermal Processes in a cooling pond. ... Numerical simulation of hydrothermal processes in lake Druksiai. ... – PowerPoint PPT presentation

Number of Views:92
Avg rating:3.0/5.0
Slides: 18
Provided by: edi25
Category:

less

Transcript and Presenter's Notes

Title: Simulation of convectiveconductiveradiative heat transfer in a cooling basin


1
Simulation of convective-conductive-radiative
heat transfer in a cooling basin
  • P. Vaitiekunas, V. Vaiis, D. Paliulis
  • Dept of Environmental Protection, Vilnius
    Gediminas Technical University, Sauletekio al.
    11, LT-10223 Vilnius-40, Lithuania
  • E-mail vaitiek_at_ap.vtu.lt, vaisisv_at_adm.vtu.lt,
    daipal_at_mail.ru
  • 2006 11 28
  • phoenics 3.6.1 VR (2004), PC Pentium 2

2
Abstract
  • The three-dimensional mathematical model of
    complex research of heat and mass transfer in
    water media was used. This allows examining the
    interaction of some transfer processes in the
    natural cooling basin (lake Drukiai) heat
    convection and conduction, direct and diffusive
    solar radiation, variable density of the water
    and heat transfer coefficient of the water-air
    interface. The combined effect of these natural
    and unnatural actions determines the heat amount
    that the basin is able to dissipate to the
    surrounding atmospheric media in thermal
    equilibrium (no change in the mean water
    temperature).
  • This article presents a number of most
    widely used expressions for vertical and
    horizontal heat transfer coefficients.
    Suggestions are made that the mixing rate at the
    water surface is caused by natural space. There
    is analyzed case when there is no wind calm.
    Mean temperature profiles measured and predicted
    in the cooling pond, as well as on their time
    variation. A comparison experimental and
    numerical result showed a qualitative agreement.

3
Content list
  • 1. Objective of work
  • 2. Description of phenomenon simulated
  • 2.1 Qualitative
  • 2.2 Mathematical
  • 3. Presentation of results
  • 4. Conclusions
  • 5. Literature References
  • 6. Non-standard nomenclature

4
Objective of the work
  • In order to qualify the cooling pond as an
    adequate thermal dissipater for the heat expelled
    by the station, will be necessary a composed
    analysis of the geographical, solar and water
    characteristics. The varying atmospheric and
    solar conditions make the basin to be a different
    characteristics dissipater everytime. Each one of
    the atmospheric or solar factors cannot determine
    by itself the dissipating capacity of the basin.
    All the elements are highly bound and must be
    treated simultaneously. The main objective is to
    establish these influences and to balance them
    with the heat coming from the nuclear power
    station. This analysis will provide us a base for
    establishing the capability of the basin to
    dissipate the heat completely or otherwise to
    calculate the net mean water temperature
    increase. The water temperature at the station
    intake will be the solution to a dynamic flowing
    and heat transfer problem that may be treated
    with PHOENICS CFD codes 1-3. We attempted to
    apply these codes in a simulation of two-phase
    mathematical model of the hydrothermal processes
    in a cooling pond, including the effects of
    three-dimensional (3D) structure features of the
    transport, power and direction of the wind,
    variable density of the water, heat conduction at
    the water-air interface, direct and diffuse solar
    radiation 4. In this paper is presented
    simulation of mass and heat transfer in a cooling
    basin according 2 but without wind blowing.

5
Phenomenon simulated

6
The lake Drukshiai with measured isoterms

7

Fig 1. Difference grid (x.y.z41.17.9)
with contours of the lake Druksiai
8
Equations solved

9
Solar radiation
10

11

12
Table 3. Numerical experiment results of basin
heat exchange
  • The results table 3, row 1, presents experiment
    which assesses all heat exchange mechanisms by
    conductivity of water-atmosphere plus radiate
    exchange atmosphere-water and wateratmosphere,
    direct and diffuse solar radiation over the basin
    surface, in the row 2 ? temperatures without
    direct solar radiation effects, 3 ? without
    diffuse solar radiation effects, 4 ? without
    estimation of radiate heat exchange
    water-atmosphere, atmosphere-water. In row 5 are
    presented measured values 5, C0, and in 6-row ?
    percentage inclination predicted temperatures of
    row 1 from measured ones.
  • yi
  • 14 12 10 8 6 4
  • 1 0C 27.77 27.96 27.56 26.12 26.08 26.20
  • 2 0C 27.59 27.56 27.36 26.04 25.90 25.96
  • 3 0C 27.73 27.91 27.51 26.10 26.03 26.15
  • 4 0C 27.77 27.96 27.55 26.12 26.08 26.20
  • 5 Exp., 0C 27.5 27.6 28.2 28.1 27.1 27.2
  • 6 Res., 0.6 0.85 ?1.9 ?4.0 ?3.8 ?3.7

13
Darbo ivada 1
  • ISC-Aermod View nusistovejusio Gauso tipo dumu
    debesies modelis.

14
4. Conclusions
  • The code of elliptic equations was used to
    construct a numerical model of hydrothermal
    dynamics in lake Druksiai, in the region of the
    hot-water discharge and heat dissipation in the
    whole basin. The CFD codes were applied for the
    numerical solution of 3D mathematical model of
    the flow and heat transfer. The solutions can
    evaluate the effect of temperature-dependent
    water density, of water-air heat conduction, of
    water mixing and of the ground geometry.
  • . Measurements and numerical simulations show a
    two-layer near field mixing structure, with the
    upper layer of the 2.5 m thickness.
  • . An analysis of the numerical solutions for the
    hydrothermal processes in lake Druksiai, and
    their comparison with the test points suggest an
    influence of the water-air heat conductivity, of
    the variable density of water, of water mixing,
    and partially of the geometry of the shore-line
    on the results of simulation, which are
    qualitatively similar to the test points.

15
5. Nomenclature
16
6. Literature References
  • 1. Montenegro H. S., Choucino M. A. (1994).
    Thermal dissipation in natural
  • Basin The PHOENICS Journal of Computational Fluid
    Dynamics its applications. Vol.7, No. 3.
    P.1436.
  • 2. Vaitiekunas P., Petkeviciene J., Katinas
    V. (1998). A Numerical simula-tion of
    three-dimensional hydrothermal Processes in a
    cooling pond. The PHOENICS Journal of
    Computational Fluid Dynamics its applications.
  • Vol. 11,
    Nr. 3. P. 348-354.
  • 3. Vaitiekunas P., Petkeviciene J., Katinas
    K. (2000). Numerical simulation of hydrothermal
    processes in lake Druksiai. Computational
    procedure. ISSN 0235-7208. Energetika. Nr.4. P.
    42-52.
  • 4. Vaitiekunas P., Petkeviciene L. (2003).
    Two-phase numerical modeling of heat exchange in
    a natural basin. In Advances in Heat Transfer
    Engine-ering, Ed. B. Sunden and J. Vilemas. 4th
    Baltic Heat Transfer Conference, 25 27 August
    2003, Kaunas, p. 435-440.
  • 5. Ecosystem of the cooling pond of the
    Ignalina NPP in the initial period of
  • its operation. T. 10. D. 1. Vilnius.
    Akademija. 1992. 246 p.

17
Thank you for atention ?
Write a Comment
User Comments (0)
About PowerShow.com